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Table 5

Summary of model parameters. For details on the parameter definitions see Robitaille et al. (2006).

3003929 3005903 3008813 3012934

Inclination 76 81 63 70 76 81 57 63 70 76
Angle [°]
SED fitting 141 189 190 153 123 151 194 199 189 188
χ 2
distance 1905 1995 2291 2291 2291 2188 2188 2188 2089 1995
 [ pc ] 
A ν 134 587 19 18 17 94 19 18 19 27
(total)
A ν 13 12 19 18 17 12 19 18 19 16
(interstellar)
stellar 4.9 5.1 5.1 5.1 5.1 5.1 4.8 4.8 4.8 4.8
radius [R ⊙ ]
stellar 15 16 16 16 16 16 14 14 14 14
mass [M]
stellar 31 000 32000 32 000 32 000 32000 32 000 31 000 31000 31 000 31 000
temperature [K]
Luminosity 20 700 25 900 25 000 25 000 25 000 25 000 17 700 17 700 17 700 17 700
(total, [L ⊙ ])
envelope accr. 0 0 0 0 0 0 0 0 0 0
rate [M/yr]
disk mass 9 × 10-2 4 × 10-2 2 × 10-2 2 × 10-2 2 × 10-2 2 × 10-2 6 × 10-2 6 × 10-2 6 × 10-2 6 × 10-2
 [ M ] 
disk inner 2 6 8 8 8 8 5 5 5 5
radius [Rsub]
disk inner 26 84 99 99 99 99 55 55 55 55
radius [AU]
disk accr. 8 × 10-08 3 × 10-6 2 × 10-7 2 × 10-7 2 × 10-7 2 × 10-7 5 × 10-7 5 × 10-7 5 × 10-7 5 × 10-7
rate [M/yr]
disk flaring 1.15 1.04 1.10 1.10 1.10 1.10 1.10 1.10 1.10 1.10
parameter β

Notes. Note that the total extinction given in the table is the sum of the interstellar and intrinsic extinction. The intrinsic extinction for disk-like structures is given for the direct line of sight; hence, it depends considerably on the inclination and flaring of the disk. If the total and interstellar extinction are equal on the other hand, this indicates a direct line of sight to the central stellar source. Robitaille et al. (2006) state that the disk structure is given by: where h ∝ ϖβ and α = β + 1.

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